[step:Use uniqueness of extensions to prove the comparison maps are inverse bijections]Let $f: S \to U(A)$ be a function. By definition of $\Psi_{S,A}$, the morphism $\Psi_{S,A}(f) = \bar f$ satisfies
\begin{align*}
U(\bar f) \circ \eta_S = f.
\end{align*}
Hence
\begin{align*}
\Phi_{S,A}(\Psi_{S,A}(f))
= \Phi_{S,A}(\bar f)
= U(\bar f) \circ \eta_S
= f.
\end{align*}
Thus $\Phi_{S,A} \circ \Psi_{S,A} = \operatorname{id}_{\mathbf{Set}(S,U(A))}$.
Conversely, let $h: F(S) \to A$ be a morphism in $\mathcal A$. The function $\Phi_{S,A}(h): S \to U(A)$ is
\begin{align*}
\Phi_{S,A}(h) = U(h) \circ \eta_S.
\end{align*}
The morphism $\Psi_{S,A}(\Phi_{S,A}(h))$ is, by definition, the unique morphism $g: F(S) \to A$ satisfying
\begin{align*}
U(g) \circ \eta_S = U(h) \circ \eta_S.
\end{align*}
But $h$ itself satisfies this same equation. By uniqueness in the free object universal property,
\begin{align*}
\Psi_{S,A}(\Phi_{S,A}(h)) = h.
\end{align*}
Therefore $\Psi_{S,A} \circ \Phi_{S,A} = \operatorname{id}_{\mathcal A(F(S),A)}$, so $\Phi_{S,A}$ is a bijection with inverse $\Psi_{S,A}$.[/step]